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Transcript
Solar Furnaces Today’s Lecture: Interiors of Stars (Chapter 12, pages 276-295) • Pre-main sequence stars • How do stars burn their fuel? • Post main-sequence evolution Pre-main-sequence stars • Relatively slow gravitational contraction, but still no nuclear reactions. • Gravitational energy still being released as the gas compresses. • When the temperature becomes sufficiently high in the center (T > 106 K), get nuclear reactions: A STAR IS BORN! • Star settles onto the main sequence and contraction ceases. The star’s L and T don’t change much during the main-sequence lifetime. • Nuclear reactions replenish energy lost from the surface, providing stability. • Star is in mechanical balance: hydrostatic equilibrium. • Hydrostatic balance does NOT require nuclear reactions. It’s just pressure balancing gravity. • But without another energy source the main sequence would be much shorter (only 30 millions years for our Sun). Brown Dwarfs: no long-term fusion • If M < 0.08 Msun, then T is not high enough for sustained nuclear reactions: get a “BROWN DWARF” (failed star) (But fusion does occur for a short time.) • It is held up by “degeneracy pressure” (quantum mechanical pressure). • Until the mid-1990s, no confirmed brown dwarfs had been found, but now there are over 1000 known. • They glow faintly at infrared wavelengths. On the main sequence • In center of a star, the temperature is very high (in the Sun, T=1.5 x 107 K). Hydrogen atoms are fully ionized, so they’re basically just protons. • Nuclear fusion produces energy. • Basic reaction is 4 1H1 --> 2He4 + energy 2 of the protons turned into neutrons + positrons (antielectrons); positrons annihilated with electrons. • 2He4 is more tightly bound (and therefore less massive) than 4 1H1, so energy is emitted. The proton-proton chain (or pp chain) On the main sequence (cont.) • 0.7% of the mass of 4 1H1 is converted to energy to produce 2He4 according to Einstein’s E = mc2. • The protons (1H1) can only overcome the electric repulsion (because they’re all positively charged) if they are moving very fast. • This means nuclear fusion requires high temperatures. (For all you quantum mechanics aficionados, it actually requires “quantum tunneling” to combine the protons.) • Energy released replenishes energy lost from surface, preventing further contraction. Sun’s Life on the Main Sequence • In the Sun, nearly 700 million tons of protons (hydrogen nuclei) are being converted to helium each second! • But there is plenty of raw material: Sun’s core has about 15% of Sun’s mass Sun is mostly hydrogen: 70% H, 28% He, 2% heavier stuff • Sun’s main-sequence life about 10 billion years! • Note that photons take about 105 years just to leak out. • All main sequence stars are fusing H to He, but in stars more massive than 1.5 Msun, the pp chain is not fast enough. How do we fuse H in this case? • The CNO cycle burns hydrogen for stars > 1.5Msun. • Carbon acts as a catalyst. It is neither created nor destroyed while turning four protons into one helium atom. Deaths of stars, 0.08Msun<M<8Msun • For 10 billions years the Sun lives happily on the main sequence. • During this time the Sun is in hydrostatic balance (gravity pulling in is balanced by pressure pushing out). • Energy is lost from the surface, but nuclear reactions provide energy to prevent contraction. • But eventually a helium core builds up to 0.1Msun, and there isn’t enough hydrogen left in the core for appreciable burning. • Contraction begin in core -> heating the star -> hydrogen burning becomes stronger in surface layers. • Star bloats to a huge size: RED GIANT! RED GIANTS! Expanding H envelope H-burning shell He Core • Contracting He core heats up --> eventually 108 K is reached 3 2He4 --> 6C12 + energy (triple-alpha process) Also 6C12 + 2He4 --> 8O16 + energy • Carbon and oxygen core forms over 106 years. BIGGER RED GIANTS! • Once again, T is too low for C/O core fusion, so the core contracts. • Off-center burning expands envelope again, creating an even larger Red Giant. H-burning shell He-burning shell CO • Depending on the mass of the star, this process can repeat, creating heavier elements. • For stars like our Sun, it becomes unstable and begins ejecting the outer layers: planetary nebula. Planetary Nebula Expanding shell of gas • Winds from the star create a planetary nebula. • The star is mostly carbon and oxygen inside, with a helium layer. Most of the hydrogen is being expelled. • An inner core of carbon and oxygen (0.6-0.9Msun) is left over, held up by “degeneracy pressure.” • This is left over as a WHITE DWARF star. CO White dwarfs • Roughly the size of the Earth with the mass of the Sun! • If you try to pack electrons into the same place they must be at different energy levels (like the energy levels of an atom). Each electron must be at a higher energy than the one before it. • All these energetic electrons in one place give rise to a pressure: ELECTRON DEGENERACY PRESSURE • This is weird stuff: one teaspoon of white dwarf weighs 3 tons! If a white dwarf is more massive, it actually has a smaller radius. • No nuclear reactions are taking place, the white dwarf just radiates its heat and continues to cool over time. • White dwarfs are sometimes used as age indicators in globular clusters. Types of White Dwarfs • The Sun will become a carbon/oxygen white dwarf with a mass of 0.6Msun. • Stars up to 8Msun become carbon/oxygen white dwarfs with masses up to ~1.1Msun. • Stars below 0.45Msun aren’t massive enough to burn helium in their core and become helium white dwarfs. • Stars with masses from 8-10Msun have an extra stage of burning in their core and make oxygen/neon/magnesium white dwarfs with masses of ~1.2Msun. • White dwarfs have a mass limit 1.4Msun (the Chandrasekhar limit), above which electron degeneracy pressure can’t hold up the star.